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Fizika Tverdogo Tela, 2025 Volume 67, Issue 4, Pages 690–696 (Mi ftt11442)

Ferroelectricity

Microstructure, dielectric and ferroelectric characteristics of 0.1BiFeO$_3$–0.9PbFe$_{0.5}$Nb$_{0.5}$O$_3$ multiferroic ceramics at temperatures of 10–850 K

A. V. Pavlenkoab, K. M. Zhidela

a Research Institute of Physics, Southern Federal University
b Southern Research Center of the Russian Academy of Sciences, Rostov-on-Don

Abstract: The microstructure, dielectric, ferroelectric and piezoelectric characteristics of the multiferroic ceramics 0.1BiFeO$_3$–0.9PbFe$_{0.5}$Nb$_{0.5}$O$_3$ have been studied. It is shown that ceramics are impurity-free and have a homogeneous grain structure. When analyzing the $\varepsilon'(T,f)$ and $\varepsilon''(T,f)$ dependences of the sample at $T$ = (10–850) K, it was found that 0.1BiFeO$_3$–0.9PbFe$_{0.5}$Nb$_{0.5}$O$_3$ is a relaxor ferroelectric; a magnetodielectric effect appears during the magnetic phase transition, and at $T>$ 450 K, a significant contribution to the dielectric response begins to be made by the Maxwell–Wagner polarization and the corresponding dielectric relaxation. It was revealed that at room temperature, 0.1BiFeO$_3$–0.9PbFe$_{0.5}$Nb$_{0.5}$O$_3$ ceramics, unlike BiFeO$_3$ and PbFe$_{0.5}$Nb$_{0.5}$O$_3$, is characterized by high values of the real part of the complex permittivity, $\varepsilon'\approx$ 9000, dielectric controllability, $K\approx$ 40% and a piezoelectric coefficient, $d_{33}\approx$ 340 pm/V.

Keywords: solid solutions, dielectric controllability, ferroelectric relaxor, Maxwell–Wagner polarization.

Received: 25.12.2024
Revised: 27.03.2025
Accepted: 28.03.2025

DOI: 10.61011/FTT.2025.04.60551.352



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